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Self –catalytic fabrication of ZnO micro and nano-tetrapods

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The ZnO materials of our case formed in the zinc-rich (oxygen- deficient) condition, especially for the positions near the source material and far from the opened en[r]

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SELF-CATALYTIC FABRICATION OF

ZnO MICRO- AND NANO-TETRAPODS

N go X u a n D a i, N g u y en T hi T hu c H ien , N g u y e n N g o c L ong

D epartm ent o f Physics, College o f Science, VN U

Abstract: Tetrapod-like zinc oxide (ZnO) micro and nanorods were produced on oxidized silicon substrates by thermal evaporation of Zn/ZnO powder mixture The synthesis procedures were carried out at 1050°c in air, and there is no arry catalyst used The fabricated ZnO tetrapods were quite uniform, high yield, good crystallinity and especially had very strong u v and green photoluminescence at room temperature The forming and photoluminescence mechanisms of the tetrapods were considered

1 In tro d u c tio n

ZnO has been realized as an excellent functional material for many fields of application Novel superstructures of ZnO, such as nano comb-, propeller-, tetrapod-, teeth­ like shapes [1-5], promise a great deal of interesting physical property, and can be used as special building blocks, components for micro/nanosystems Recently, in the world, many attempts have been made to synthesize, characterize and apply ZnO tetrapod-like structures [2-5] Authors of [2] found that the sintering temperature of their ZnO-glass varistors were evidently lowered because of the higher activity of tetrapod (TP) ZnO nanopowders Low-field electron emission and the technological usefulness of ZnO TPs synthesized by rapid heating of zinc pellet was reported in [3] Room-temperature photoluminescence (PL) of ZnO TPs prepared by oxidation of zinc powders [4] or evaporation of ZnC 03 powder [5] was clearly observed and it showed the potential ability for fabricating light-emitting devices in nanoscale optoelectronics For the nice application prospects, the synthesis procedures, forming mechanisms and physical properties of ZnO TPs are continuatively studied and developed.

In this paper, we report our efficient route for synthesis ZnO TPs and the beginning discussion on their structural, photoluminescence properties.

2 E x p e rim e n ta l

Our synthesis method is based on a vapor

transport process and a simple experiment setup shown

in figure 1 The source material for evaporation is a

mixture of high purity zinc metal (Zn) and zinc oxide

(ZnO) powders (molar ratio 2:1) The source material

and the SiO^Si substrates were placed inside a quartz

tube, the source material was located at the closed end

while the substrates were arranged toward the opened

end of the tube The quartz tube was inserted to a

horizontal furnace in air ambient The temperature of the source material was ~1050°c, of

Furnace quarzttube

source material substrates

F ig l Experiment setup for synthesis of ZnO tetrapods

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Self-catalytic fabrication of 3 9

the substrates was in range 850-:-950°C The temperature was kept for 1.5 hour, and then naturally cooled down to room temperature After the experiment, white fluffy products of mass yield were found on the substrates and the quartz tube The products covered on the substrates were collected for characterization Morphology and crystal structure of the products were characterized bv scanning electron microscopy (SEM) (JEOL JSM 5410 LV) and X-ray diffractometer (Brucker D5005) Photoluminescence of the samples were recorded by a spectrofluorometer (FL3-22 Jobin-Yvon).

3 R e su lts a n d d is c u s s io n

X-ray diffraction (XRD) patterns of the

synthesized products show characteristic diffraction

peaks of hexagonal wurzite ZnO crystal phase, there

is no any diffraction signal of impurity (fig.2).

The typical SEM image shown in fig.3

illustrates the tptrapod-like shape of the synthesized

ZnO products Each tetrapod is composed of four ZnO

micro/nanorods - legs of tetrapods - with the diameter

o f about 500-7-2000 nm and length of several

micrometers, this sizes depend on the location of the

substrate in the quartz tube of the synthesis process.

All the legs o f the TPs have smooth surface and

particularly have hexagon end planes, as can be

seen in the SEM image (fig 3).

Hexagonal wurzite cell of ZnO presents a

polar oxide (or zinc) {001] plane and an electrically-

neutral non-polar [100] plane, as shown in the inset

picture of figure 2 The polar plane is metastable

and thus favors a fast growth rate, while the non­

polar face has higher stability Ị6Ị We believe that in

our synthesis conditions ZnO nuclei formed in the

typical hexagonal wurzite structure and fast grew

up layer-by-layer along the c-axis (<0001>),

therefore resulted in hexagonal shape, end planes

and single crystalline of the legs of the ZnO TPs.

Both vapor-liquid-solid (VLS) and vapor-solid

synthesis procedures because at the synthesis temperature (850-950"C), ZnO solids, ZnOx (x<l), Zn liquids could exist together and play as the self-catalysts for the growth of ZnO micro/nanorods (the legs of TPs) [1, 5], However, the v s mechanism may dominate due to that Zn and ZnO, liquid droplets (with boiling point of 907°C) easily transit to gaseous state

at the synthesis temperature The explanation for the forming of the tetrapod-like morphology is still an exciting problem for worldwide research May be, the volcanic oxidation of Zn powder plays an important role leading to the growth of the ZnO TPs Four

2 theta degree Fig.2 XRD pattern of ZnO tetrapod products ; The inset is the hexagonal unit cell of ZnO [6]

Fig 3 A typical SEM image of the synthesized ZnO products (VS) processes could occur in our

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4 0 Ngo Xuan Dai, Nguyen Thi Thuc Hien, Nguyen Ngoc Long

Room-temperature photoluminescence spectra of

the ZnO TPs excited with a 335 nm light (from a 450W

Xenon lamp) were shown in Fig 4 Very inten se

emission peaks at 388 nm (UV) and 495 nm (green)

were observed in all the synthesized samples The first

narrow peak at 388 nm can be attributed to excitonic

recombination This u v peak is red shift in comparison

with the 380 nm peak of usual cases of ZnO The broad

peak at 495 nm is mainly due to oxygen vacancies

(inducing deep levels) in the ZnO crystals [7] The ZnO

materials of our case formed in the zinc-rich (oxygen-

deficient) condition, especially for the positions near the

source material and far from the opened end (air

ambient) of the synthesis quartz tube (fig 1) The

further distance from the opened end of the tube, the

higher probability of forming oxygen vacancies, thus the

green emission increases and the ƯV emission is

partially quenched (fig 4) The representative excitation

spectrum of the 495 nm emission peak (fig.5) indicates

the optical semiconductor nature of the ZnO TPs with

the clea r excito nic absoi'ption peak a t 381 nm G ood

excitonic optical transitions can reveal the high purity

and good crystallinity of the ZnO products.

4 S um m ary

We have fabricated tetrapod-like ZnO micro/nanorods by a sim ple experiment setup The synthesis process, forming mechanism and physical properties of the ZnO tetrapods are still the land for active researches in coming time Very high intense ultra-violet and green photoluminescence at room temperature of our synthesized ZnO tetrapods exposes the potential for fabricating micro and nanoscale light-em itting devices.

R eferen ces:

1 Peidong Yang, Haoquan Yan, s Mao, R Russo, J Johnson, R Saykally, N Morris J

Pham, R He, H Choi, Adv Fund Mater 12, No.5(2002), 323.

2 Wu Jun, Xie Changsheng Bai Zikui, Zhu Bailin, Huang Kaijin, Wu Run, Mater Sci Eng

B95(2002) 157.

3 Q Wan K Yu , T.H Wang, C L L in , Appl Phys Lett., 83(2003), 2253

4 Y.Dai, Y Zhang, Q.K Li, c w Nan, Chem Phys Lett, 358(2002) 83.

5 w D.Yu, X M Li, X D Gao, Appl Phys Lett, 84(2004) 2658.

6 L Znaidi G.J.A.A Illia s Benyaha, c Sanchez, A.v Kanaev, T hin Solid Films, 428(2003).

257

7 K Vanheusden, W.L Warren, C.H Seager, D.R Tallant, J A Voigt, J Appl Phys, 79(10),

(1996), 7983.

381 nm

wavelength nm

Fig.5 Excitation spectrum of the synthesized ZnO TPs

wavelength nm

Fig.4 P L spectra o f the ZnO TP s formed near (solid line) and far from (dotted line) the opened end

of the quartz tube

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